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CIE 9231 2026 June Paper 13 Q7

A Level / CIE / FP1

CIE 9231 2026 June Paper 13 Paper · Question 7

题目

Problem

The plane Π\Pi has equation r=j+2k+s(i−j)+t(−3i+j−k)\mathbf{r}=\mathbf{j}+2\mathbf{k}+s(\mathbf{i}-\mathbf{j})+t(-3\mathbf{i}+\mathbf{j}-\mathbf{k}).

(a) Obtain an equation of Π\Pi in the form ax+by+cz=dax+by+cz=d.

(4)

(b) The point PP has position vector (6+6θ)i+(1+θ)j+(2+5θ)k(6+6\theta)\mathbf{i}+(1+\theta)\mathbf{j}+(2+5\theta)\mathbf{k}.

Find the set of values of θ\theta for which the perpendicular distance of PP from Π\Pi is less than 6\sqrt{6}.

(4)

(c) Find an equation for the common perpendicular to the lines

r= λ(j+2k)andr= i+2k+μ(−3i+j−k).\begin{align*} \mathbf{r}=&\,\lambda(\mathbf{j}+2\mathbf{k})\quad\text{and}\\ \mathbf{r}=&\,\mathbf{i}+2\mathbf{k}+\mu(-3\mathbf{i}+\mathbf{j}-\mathbf{k}). \end{align*}
(8)
题目中文翻译

平面 Π\Pi 的方程为 r=j+2k+s(i−j)+t(−3i+j−k)\mathbf{r}=\mathbf{j}+2\mathbf{k}+s(\mathbf{i}-\mathbf{j})+t(-3\mathbf{i}+\mathbf{j}-\mathbf{k})。

(a) 求 Π\Pi 的方程,写成 ax+by+cz=dax+by+cz=d 的形式。

(4)

(b) 点 PP 的位置向量为 (6+6θ)i+(1+θ)j+(2+5θ)k(6+6\theta)\mathbf{i}+(1+\theta)\mathbf{j}+(2+5\theta)\mathbf{k}。

求使 PP 到 Π\Pi 的垂直距离小于 6\sqrt{6} 的 θ\theta 值的集合。

(4)

(c) 求下列两条直线的公垂线方程:

r= λ(j+2k),r= i+2k+μ(−3i+j−k).\begin{align*} \mathbf{r}=&\,\lambda(\mathbf{j}+2\mathbf{k}),\\ \mathbf{r}=&\,\mathbf{i}+2\mathbf{k}+\mu(-3\mathbf{i}+\mathbf{j}-\mathbf{k}). \end{align*}
(8)
原卷通用作答要求

Answer all questions. You should use a calculator where appropriate.

You must show all necessary working clearly; no marks will be given for unsupported answers from a calculator.

Give non-exact numerical answers correct to 3 significant figures, or 1 decimal place for angles in degrees, unless a different level of accuracy is specified in the question.

请回答所有题目。适当时应使用计算器。必须清楚展示所有必要的计算过程;仅给出计算器答案而没有过程,不予评分。除非题目另有精度要求,非精确数值答案保留 3 位有效数字,以度为单位的角度保留 1 位小数。

解答

(a)

解法一

思路

展开

用两条平面内方向的叉积求法向量,再代入平面上给定点确定常数。

答题过程

展开

Two direction vectors in Π\Pi are u=(1,−1,0)\mathbf u=(1,-1,0) and v=(−3,1,−1)\mathbf v=(-3,1,-1). A normal is

n=u×v=(1,1,−2).\mathbf n=\mathbf u\times\mathbf v=(1,1,-2).

The plane contains (0,1,2)(0,1,2), so its equation is

x+y−2z=0+1−2(2),x+y−2z=−3.x+y-2z=0+1-2(2), \qquad\boxed{x+y-2z=-3}.

(b)

解法一

思路

展开

代入点到平面的距离公式,再解严格绝对值不等式;平面方程常数项的符号要特别注意。

答题过程

展开

The perpendicular distance is

d= ∣6+6θ+1+θ−4−10θ+3∣6= ∣6−3θ∣6.\begin{align*} d=&\,\frac{|6+6\theta+1+\theta-4-10\theta+3|}{\sqrt6} \\[4mm] =&\,\frac{|6-3\theta|}{\sqrt6}. \end{align*}

Hence d<6d<\sqrt6 is equivalent to

∣6−3θ∣<6,−6<6−3θ<6.|6-3\theta|<6, \qquad -6<6-3\theta<6.

Solving gives 0<θ<4\boxed{0<\theta<4}.

(c)

解法一

思路

展开

设两条线上的点Q、R,公垂线连接向量同时垂直于两方向。解参数后用最近点与公垂线方向写直线方程。

答题过程

展开

Let

Q= (0,λ,2λ),R= (1−3μ,μ,2−μ)\begin{align*} Q=&\,(0,\lambda,2\lambda),\\[4mm] R=&\,(1-3\mu,\mu,2-\mu) \end{align*}

lie on the first and second lines, respectively. Then

QR→=(1−3μ,μ−λ,2−μ−2λ).\overrightarrow{QR}=(1-3\mu,\mu-\lambda,2-\mu-2\lambda).

For QRQR to be perpendicular to both lines,

QR→⋅(0,1,2)= 0,QR→⋅(−3,1,−1)= 0.\begin{align*} \overrightarrow{QR}\cdot(0,1,2)=&\,0, \\[4mm] \overrightarrow{QR}\cdot(-3,1,-1)=&\,0. \end{align*}

These give

μ+5λ= 4,11μ+λ= 5.\begin{align*} \mu+5\lambda=&\,4,\\[4mm] 11\mu+\lambda=&\,5. \end{align*}

From λ=5−11μ\lambda=5-11\mu, substitution gives μ+25−55μ=4\mu+25-55\mu=4, so

μ=718,λ=1318.\mu=\frac7{18},\qquad\lambda=\frac{13}{18}.

Therefore

R=118(−3,7,29),QR→=−16(1,2,−1).R=\frac1{18}(-3,7,29), \qquad\overrightarrow{QR}=-\frac16(1,2,-1).

The common perpendicular is

r= 118(−3i+7j+29k) +t(i+2j−k),t∈R.\begin{align*} \mathbf r=&\,\frac1{18}(-3\mathbf i+7\mathbf j+29\mathbf k)\\[4mm] &\,+t(\mathbf i+2\mathbf j-\mathbf k),\qquad t\in\mathbb R. \end{align*}

Its direction has zero dot product with (0,1,2)(0,1,2) and (−3,1,−1)(-3,1,-1), and it passes through the calculated points on both lines.